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- W2100067268 abstract "Artificial pinning centers have been introduced into high-T <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>C</sub> superconducting films in order to improve the J <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>C</sub> at 77 K and magnetic fields. The dimensionality of artificial pinning centers has an important role in improving J <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>C</sub> against the magnetic field direction. The one-dimensional artificial pinning centers, such as dislocations and nanorods, are much effective on the B//c-axis. However, pinning centers with magnetic angular independences are much important for practical use. Then, a new concept of zero-dimensional artificial pinning centers is applied to high-T <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>C</sub> superconducting films, which is local superconductivity disappearance resulting in the substitution of 3d-transition elements such as Zn or Co for Cu. We have no clear evidence of element substitution from microstructural observations. However, the magnetic field angular independences in a wide region except the B//a-axis are revealed in a Zn-doped film, which probably results form zero-dimensional pinning centers. Unexpected magnetic field angular dependences are also revealed, indicating the existence of other pinning centers except zero-dimensional pinning centers. It is found that unexpected defects, such as c-axis-correlated defects or stacking faults, are induced by 3d-transition element substitution." @default.
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- W2100067268 date "2007-06-01" @default.
- W2100067268 modified "2023-10-16" @default.
- W2100067268 title "Microstructures of High-${rm T}_{rm C}$ Superconducting Films Introduced Zero-Dimensional and One-Dimensional Artificial Pinning Centers" @default.
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- W2100067268 doi "https://doi.org/10.1109/tasc.2007.898168" @default.
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